Linear Motion free study note

(a) Uniform Linear Motion

  • Velocity remains constant
  • Acceleration is zero

Example:

  • A car moving at constant speed on a straight road

(b) Non-Uniform Linear Motion

  • Velocity changes with time
  • Acceleration is not zero

Example:

  • A freely falling body
  • A vehicle accelerating or decelerating

(a) Position

The location of a particle with respect to a fixed reference point.

(b) Displacement

Displacement is the change in position of a body in a particular direction.

  • Vector quantity
  • Can be positive or negative

Displacement=Final positionโˆ’Initial position\text{Displacement} = \text{Final position} – \text{Initial position}

(c) Distance

  • Total length of the path travelled
  • Scalar quantity
  • Always positive

(d) Velocity

Velocity is the rate of change of displacement with respect to time.Velocity=dsdt\text{Velocity} = \frac{ds}{dt}

  • Unit: m/s
  • Vector quantity

(e) Speed

  • Magnitude of velocity
  • Scalar quantity

(f) Acceleration

Acceleration is the rate of change of velocity with respect to time.Acceleration=dvdt\text{Acceleration} = \frac{dv}{dt}

  • Unit: m/sยฒ
  • Can be positive (acceleration) or negative (retardation)

When acceleration is constant, the motion is called uniformly accelerated motion.

Equations of Motion

For constant acceleration:

v=u+atv = u + at

s=ut+12at2s = ut + \frac{1}{2}at^2

v2=u2+2asv^2 = u^2 + 2as

Where:

  • uuu = Initial velocity (m/s)
  • vvv = Final velocity (m/s)
  • aaa = Acceleration (m/sยฒ)
  • ttt = Time (s)
  • sss = Displacement (m)

Motion under gravity is a special case of linear motion where:

  • Acceleration = g=9.81โ€‰m/s2g = 9.81 \, m/s^2

Free Fall

  • Initial velocity u=0u = 0
  • Acceleration a=ga = g

Equations become:v=gtv = gts=12gt2s = \frac{1}{2}gt^2

Retardation is negative acceleration, meaning velocity decreases with time.

Example:

  • Application of brakes in a vehicle

a=vโˆ’ut(a<0)a = \frac{v – u}{t} \quad (a < 0)

Relative motion considers the motion of one body with respect to another moving body.

If:

  • Velocity of A = vAv_A
  • Velocity of B = vBv_B

Then:Relative velocity of A w.r.t B=vAโˆ’vB\text{Relative velocity of A w.r.t B} = v_A – v_B

Used in:

  • Train problems
  • Vehicle overtaking problems

Linear motion is widely used in:

  • Machine design
  • Piston-cylinder mechanisms
  • Elevators and lifts
  • Structural analysis
  • Vehicle dynamics
  • Sliding of blocks on inclined planes
  • Motion of piston in IC engines
  • Vertical motion of cranes
  • Conveyor belt systems

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